electroweak interactions topical group
TRANSCRIPT
Electroweak Interactions Topical Group
Conveners
Wolfgang Kilian, University of SiegenTheory
Taikan Suehara, Kyushu UniversityExperiment
Graham Wilson, University of KansasExperiment
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The e+e− LandscapeILC: polarized e− (80%) and e+ (30%). No trigger needed. Use all decay modes.
Unpolarized cross-sections
Study electroweak physics with 2f, 4f, 6f, 8f. Ranging from the Z-pole to√s
conceivably around 1 TeV. Expect ZH, WWZ, WWH, ZZZ, ZZH, ZHH, tt,WWWW, WWZZ, ttH within reach of 500 GeV collider.
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Electroweak Physics Channels
Di-fermion production, e+e− → ff with f = e, µ, τ, q (q=u,d,s,c,b,t)
Radiative di-fermion production, e+e− → ffγ.Especially µ+µ−γ, ννγ and qqγ.
Di-boson production. Mainly 4-fermion final states resulting from WW, ZZ,ZH, but also Zγ, γγ.
Multiple-boson production. Mainly 6-fermion final states (from WWZ,WWH, ZZZ, ZZH, ZHH), but also WWγ, ZHγ, Zγγ.
Other processes. 4f: single Z, (eeZ and ννZ), single W (Weνe). ννγγ etc.
Quartic boson production
Alternative collider modes (e−e−, e−γ and γγ)
1 Zf f couplings
2 WWγ and WWZ trilinear couplings
3 quartic couplings (WWWW, WWZZ, WWZγ and WWγγ)
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Some Physics Goals and Questions I
Z couplings to fermions
Study the potential improvements in Z observables from a dedicated Z polerun with polarized beams and line-shape scan. Evaluate detector andaccelerator requirements. Key issue: excellent understanding of
√s scale.
Utility of radiative return events for Z physics?
How can precision Z couplings test BSM models?
Importance of polarized observables (key asset of ILC)
How can 2-fermion measurements at the highest energies constrain newphysics?
Are final-state polarization measurements with tau leptons important at thehighest energies? Quantify related detector requirements.
· · ·
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Some Physics Goals and Questions II
WW program
Define the ILC experimental program on W boson pair production. What arethe key observables and detector requirements?
What are the various ways to measure the W boson mass at the ILC andultimate precision? Is a run at threshold well motivated?
How can one best achieve a precision measurement of the W width?
Can ILC measure the polarized production amplitudes in a modelindependent way?
What BSM models are tested by this program?
What advances in theory are needed to fully exploit 108 WW events?
Can one fully utilize massive gauge boson reconstruction in hadronic decays?
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Some Physics Goals and Questions III
Other weak boson processes and generic questions
What are the ILC capabilities to study the other weak boson reactionsincluding triple-boson, four-boson production and vector-boson scattering?
Can all the various processes be analyzed coherently with the other EWmeasurements including in global fits.
How well can the quartic couplings be isolated and measured?
Explore the complementarity of the direct multi-boson production with VBS
Direct CKM matrix element measurements from W decays
Rare decays of the W
Lepton universality tests in W decays, Z decays, and tau decays
Does the Z couple to uu/dd/ss/cc/bb as described in SM?
Can WW and ZZ be used to learn about color reconnection?
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Concluding Remarks
Relations to other topical groups and task forces
Almost all of the task forces will be very pertinent to EW physics
Some overlap/cross-talk of course with other groups
Questions
Many interesting questions to explore
What interests you? Do you have ideas on complementary topics?
Invitation
We welcome experimentalists and theorists to join:
share your perspective
better understand the capabilities of the ILC for electroweak physics
inform the detector and accelerator design
Recent documentation on physics ideas, SM tests, and the ILC project in Refs. [1, 2, 3]
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References I
[1] K. Fujii et al., [LCC Physics Working Group],ILC Study Questions for Snowmass 2021, arXiv:2007.03650
[2] K. Fujii et al. [LCC Physics Working Group],Tests of the Standard Model at the International Linear ColliderarXiv:1908.11299
[3] P. Bambade et al.The International Linear Collider: A Global Project, arXiv:1903.01629
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